Please use this identifier to cite or link to this item: https://scholarbank.nus.edu.sg/handle/10635/91629
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dc.titlePhotoconductivity in poly[[o-(trimethylsilyl)phenyl]acetylene]
dc.contributor.authorKang, E.T.
dc.contributor.authorNeoh, K.G.
dc.contributor.authorMasuda, T.
dc.contributor.authorHigashimura, T.
dc.contributor.authorYamamoto, M.
dc.date.accessioned2014-10-09T08:20:22Z
dc.date.available2014-10-09T08:20:22Z
dc.date.issued1989-07
dc.identifier.citationKang, E.T.,Neoh, K.G.,Masuda, T.,Higashimura, T.,Yamamoto, M. (1989-07). Photoconductivity in poly[[o-(trimethylsilyl)phenyl]acetylene]. Polymer 30 (7) : 1328-1331. ScholarBank@NUS Repository.
dc.identifier.issn00323861
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/91629
dc.description.abstractSteady-state photoconductivity was studied in thin films of poly[[o-(trimethylsilyl)phenyl]acetylene], or poly(o-Me3SiPA) sandwiched between SnO2 and metal electrodes. Both the dark current density (Jd) and photocurrent density (Jph) depend superlinearly on the applied electric field. Jph also shows a superlinear dependence on light intensity. However, Jd and Jph are only weak functions of temperature at temperatures below room temperature. We conclude that the photoconductivity in poly(o-Me3SiPA) arises mainly from trap-modulated carrier photoemission from electrodes and the polymer is capable of effective transport of holes. © 1989.
dc.sourceScopus
dc.subjecthole transport
dc.subjectphotoconductivity
dc.subjectpoly[[o-(trimethylsilyl)phenyl]acetylene]
dc.subjectthin film
dc.typeArticle
dc.contributor.departmentCHEMICAL ENGINEERING
dc.description.sourcetitlePolymer
dc.description.volume30
dc.description.issue7
dc.description.page1328-1331
dc.description.codenPOLMA
dc.identifier.isiutNOT_IN_WOS
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